In this paper, the XPS study of SnO2 thin films deposited by the L-CVD technique are presented. The influence of exposition of the as-deposited samples to oxygen O2 and hydrogen H2 on their stoichiometry was determined. Moreover, on the basis of detailed shape analysis of the Sn3d5/2 and O1s XPS peaks, the chemical shift of binding energy corresponding to the change of sample stoichiometry was separated from a shift of the binding energy corresponding to the change of interface Fermi level position EF-Ev in the band gap, using a new procedure of deconvolution of the core level XPS peaks. The shift of the Sn3d5/2 peak by approximately 0.5 eV towards the lower binding energy after highest H2 exposure was interpreted as a true chemical shift due to an increase of Sn2+ component, whereas the shift of Sn3d5/2 peak and O1s peak after highest O2 exposure by approximately 0.5 eV towards the lower binding energy was interpreted as a result of the shift of the interface Fermi level position in the band gap towards the top of valence band at the surface, which corresponds to a deep accumulation layer typical for SnO2 thin films. © 2001 Elsevier Science B.V.

XPS study of the L-CVD deposited SnO2 thin films exposed to oxygen and hydrogen

Larciprete;
2001

Abstract

In this paper, the XPS study of SnO2 thin films deposited by the L-CVD technique are presented. The influence of exposition of the as-deposited samples to oxygen O2 and hydrogen H2 on their stoichiometry was determined. Moreover, on the basis of detailed shape analysis of the Sn3d5/2 and O1s XPS peaks, the chemical shift of binding energy corresponding to the change of sample stoichiometry was separated from a shift of the binding energy corresponding to the change of interface Fermi level position EF-Ev in the band gap, using a new procedure of deconvolution of the core level XPS peaks. The shift of the Sn3d5/2 peak by approximately 0.5 eV towards the lower binding energy after highest H2 exposure was interpreted as a true chemical shift due to an increase of Sn2+ component, whereas the shift of Sn3d5/2 peak and O1s peak after highest O2 exposure by approximately 0.5 eV towards the lower binding energy was interpreted as a result of the shift of the interface Fermi level position in the band gap towards the top of valence band at the surface, which corresponds to a deep accumulation layer typical for SnO2 thin films. © 2001 Elsevier Science B.V.
2001
Binding energy
Chemical vapor deposition
Energy gap
Fermi level
Gas adsorption
Hydrogen
Oxygen
Semiconducting tin compounds
Stoichiometry
Thin films
X ray photoelectron spectroscopy
Chemical shift
Semiconducting films
File in questo prodotto:
Non ci sono file associati a questo prodotto.

I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.

Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/243762
Citazioni
  • ???jsp.display-item.citation.pmc??? ND
  • Scopus 251
  • ???jsp.display-item.citation.isi??? ND
social impact